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Idea

An nn-fold iterated loop space Ω nX\Omega^n X canonically carries the structure of an E n E_n -algebra (an algebra over the little n-disk operad 𝒞 n\mathcal{C}_n) with Sym ( k ) Sym(k) -equivariant structure maps

𝒞 n(k)× Sym(k)(Ω nX) kμ kΩ nX. \mathcal{C}_n(k) \times_{Sym(k)} \big( \Omega^n X \big)^k \overset{\mu_k}{\longrightarrow} \Omega^n X \,.

Passing to ordinary homology of the loop space with coefficients in a finite field, H (Ω nX;𝔽 p)H_\bullet\big( \Omega^n X; \mathbb{F}_p \big), the Dyer-Lashof operations are essentially the pushforward/images in homology under the binary operation μ 2\mu_2

H (𝒞 n(2)× Sym(2)(Ω nX) 2;𝔽 p)(μ 2) *H (Ω nX;𝔽 p). H_\bullet\big( \mathcal{C}_n(2) \times_{Sym(2)} (\Omega^n X)^2 ; \mathbb{F}_p \big) \overset { (\mu_2)_\ast } {\longrightarrow} H_\bullet\big( \Omega^n X; \mathbb{F}_p \big) \mathrlap{\,.}

or rather, this map precomposed with

H i(𝒞 n(2)/Sym(2);𝔽 p)×H q(Ω nX;𝔽 p) H i+2q(𝒞 n(2)× Sym(2)(Ω nX) 2;𝔽 p) (e i,x) e i(xx). \begin{array}{ccc} H_i\big( \mathcal{C}_n(2)/Sym(2) ; \mathbb{F}_p \big) \times H_q\big( \Omega^n X ; \mathbb{F}_p \big) & \overset {\phantom{-} \boxtimes \phantom{-}} {\longrightarrow} & H_{i + 2 q}\big( \mathcal{C}_n(2) \times_{Sym(2)} (\Omega^n X)^2 ; \mathbb{F}_p \big) \\ (e_i, x) &\mapsto& e_i \boxtimes (x \otimes x) \mathrlap{\,.} \end{array}

Now,

𝒞 n(2) Conf 2( n) S n1 \begin{aligned} \mathcal{C}_n(2) & \simeq Conf_2\big(\mathbb{R}^n\big) \\ & \simeq S^{n-1} \end{aligned}

is equivalently the configuration space of 2 points in n\mathbb{R}^n, which in turn is equivalently the ( n 1 ) (n-1) -sphere of directions between these two points. Therefore

𝒞 n(2)/Sym(2)P n1 \mathcal{C}_n(2) \big/ Sym(2) \simeq \mathbb{R}P^{n-1}

is equivalently the real projective space.

For p=2p=2, the ordinary homology of this space is (cf. there and use the universal coefficient theorem):

H i(P n1;𝔽 2){𝔽 2 for0in1 0 otherwise. H_i\big( \mathbb{R}P^{n-1}; \mathbb{F}_2 \big) \simeq \left\{ \begin{array}{ll} \mathbb{F}_2 & \;\text{for}\; 0 \leq i \leq n-1 \\ 0 & \text{otherwise.} \end{array} \right.

Therefore there is a unique homology generator e ie_i in each degree up to n1n-1.

Finally, the Dyer-Lashof operations Q iQ_i at the even prime are the above homology maps indexed by these generators:

H q(Ω nX;𝔽 2) Q i H i+2q(Ω nX;𝔽 2) x (μ 2) *(e i(xx)). \begin{array}{ccc} H_q\big( \Omega^n X ; \mathbb{F}_2 \big) &\overset{\phantom{-}Q_i\phantom{-}}{\longrightarrow}& H_{i + 2q}\big( \Omega^n X ; \mathbb{F}_2 \big) \\ x &\mapsto& (\mu_2)_\ast\big( e_i \boxtimes (x \otimes x) \big) \mathrlap{\,.} \end{array}

References

The original articles:

Further early discussion:

The modern reformulation via operads is hinted at in

and expanded on in:

Review:



Γt:AΓextract(t):AΓt:Ax:Au:BΓletboxx=tinu:B \frac{\Gamma \vdash t:\Box A}{\Gamma \vdash \mathsf{extract}(t):A} \qquad \frac{\Gamma \vdash t : \Box A \qquad x : A \vdash u : B}{\Gamma \vdash \mathsf{let\ box}\ x = t\ \mathsf{in}\ u : B}

ʃ\esh

J= if iθ i+ jg jdθ jf i,g jC (X). J \;=\; \sum_i f_i \theta_i + \sum_j g_j d \theta_j f_i, g_j \in C^\infty(X) \,.

Last revised on May 25, 2026 at 17:17:12. See the history of this page for a list of all contributions to it.